Bounds for Rayleigh-Bénard convection between free-slip boundaries with an imposed heat flux
arXiv:1709.08932 · doi:10.1017/jfm.2017.907
Abstract
We prove the first rigorous bound on the heat transfer for three-dimensional Rayleigh-Bénard convection of finite-Prandtl-number fluids between free-slip boundaries with an imposed heat flux. Using the auxiliary functional method with a quadratic functional, which is equivalent to the background method, we prove that the Nusselt number is bounded by uniformly in the Prandtl number, where is the Rayleigh number based on the imposed heat flux. In terms of the Rayleigh number based on the mean vertical temperature drop, , we obtain . The scaling with Rayleigh number is the same as that of bounds obtained with no-slip isothermal, free-slip isothermal, and no-slip fixed flux boundaries, and numerical optimization of the bound suggests that it cannot be improved within our bounding framework. Contrary to the two-dimensional case, therefore, the -dependence of rigorous upper bounds on the heat transfer obtained with the background method for three-dimensional Rayleigh-Bénard convection is insensitive to both the thermal and the velocity boundary conditions.
5 pages, 3 figures. Version 2: changed format to JFM, minor rewriting following comments by referees, added Appendix A
References in corpus (3)
Cited by in corpus (10)
- The background method: Theory and computations
- A Framework for Input-Output Analysis of Wall-Bounded Shear Flows
- Analytical bounds on the heat transport in internally heated convection
- Pressure-driven flows in helical pipes: bounds on flow rate and friction factor
- Optimal cooling of an internally heated disc
- Interaction between forced and natural convection in a thin cylindrical fluid layer at low Prandtl number
- Internal heating profiles for which downward conduction is impossible
- Rigorous bounds on the heat transport of rotating convection with Ekman pumping
- Internally heated convection with rotation: bounds on heat transport
- Experimental study of the convection in a thin cylindrical gas layer with imposed bottom and top fluxes and imposed side temperature